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Regularity of minimizers for double phase functionals of borderline case with variable exponents

  • Maria Alessandra Ragusa and Atsushi Tachikawa EMAIL logo
Published/Copyright: June 13, 2024

Abstract

The aim of this article is to study regularity properties of a local minimizer of a double phase functional of type

( u ) Ω ( D u p ( x ) + a ( x ) D u p ( x ) log ( e + D u ) ) d x ,

being p ( x ) , a ( x ) log-continuous functions with p ( x ) > 1 , a 0 . Double phase functionals ( D u p + a ( x ) D u q ) d x , with constant exponents p and q ( q p 1 ) , appeared in the papers by Zhikov, and C 1 , α -regularity of their minimizers was given by Colombo and Mingione. Later, by Baroni, Colombo, and Mingione, the above type functionals with logarithm but with constant exponent, regularity properties were given. They obtained sharp regularity results for minimizers of such functionals. In this article, we treat the case that the exponents are functions of p ( x ) and partly generalize their regularity results.

MSC 2010: 35J20; 35J47; 35J60; 49N60

1 Introduction and main theorem

In this article, we show interior regularity results for minimizers of the so-called double phase functionals of borderline case with variable exponents.

Typical example of double phase functionals is given by

P p , q ( u ; Ω ) Ω ( D u p + a ( x ) D u q ) d x ,

where q > p > 1 and a ( x ) 0 . The following type of functional is treated by Baroni et al. [7]:

(1.1) P log ( u ; Ω ) Ω ( D u p + a ( x ) D u p log ( e + D u ) ) d x .

According to the title of [7], let us call P log double phase functionals “of borderline case.” Recently, Baroni and Coscia [9] treated a type of generalized functional of P log . Their generalization is of a different type than ours.

These kinds of functionals are typical example of the so-called nonstandard or ( p , q ) -growth functionals introduced by Marcellini [40]. When we consider u : Ω R n R N ( n 2 , N 1 ) a functional

u f ( x , u , D u ) d x , λ z p f ( x , u , z ) Λ ( 1 + z ) q , q p 1 , Λ λ > 0 ,

we call it a functional of standard growth if p = q , and nonstandard or ( p , q ) -growth if q > p . By Marcellini’s early papers [4042] many essential results for the regularity of minimizers of non-standard functionals have been already given. However, the category of non-standard functionals is very general and broad, and for variational problems for such functionals we cannot apply naively standard regularity theory established for uniformly elliptic problems. Therefore, many unsolved regularity problems remain until now.

The functional P p , q has, originally, developed in homogenization theory and it is connected to the well-known Lavrentiev phenomenon, see for example [53]. Double phase functionals appeared, also, in the papers by Zhikov [5456].

We are interested in the study of regularity problems and remark that this kind of functionals is both useful and compelling, because it belongs to the category of non-standard growth functionals.

The double phase functionals change their growth order with respect to D u at zero-points of a ( x ) . Indeed, we observe that the functional P p , q is a non-standard ( p , q ) -growth functional having, if a > 0 , q -growth in the gradient term, while, if a = 0 , p -growth in the gradient term. As pointed out in many previous articles, (see, for example, [12,14,26]), this is the principal characteristic of this class of functionals useful to describe the behavior of strongly anisotropic materials whose hardening properties, changing the point, can be strongly different. This considerable phase transition problem is represented by the functional P p , q , where the control of the mixture between two different materials, with p and q hardening, is governed by the term a ( ) , but this quantity, in the meantime, brought new difficulties in the regularity theory.

We point out that everywhere C 1 , α - (or even C 0 , α -) regularity problem for the double phase problems has been without solution for several decades. The first answer in this direction was given by Colombo and Mingione in [12]. Other regularity results involving double phase functionals are obtained by Colombo and Mingione in the paper [13], where the fundamentals of the double phase regularity theory have been settled, and by Baroni, Colombo, and Mingione, e.g. in [68,13,14]. Particularly, in the last mentioned paper, they provide a systematic regularity theory for the functional (1.1). For minimizers u of P log , they obtained Hölder continuity assuming logarithmic continuity of a ( ) , and C 1 , α -regularity assuming Hölder continuity of a ( ) . More precisely, a significant model example with non-standard double phase growth is treated obtaining the following result.

Theorem

(Baroni et al. [7, Theorem 2.4, 6.1]) For n 2 , N 1 , p > 1 , and a bounded domain Ω R n let u W 1 , 1 ( Ω ; R N ) be a local minimizer of P log defined in (1.1) and assume that the function a ( ) is non-negative and bounded. Let ω ( ) be its modulus of continuity in the sense that

a ( x ) a ( y ) ω ( x y ) f o r e v e r y x , y Ω ,

and denote

limsup r 0 ω ( r ) log 1 r l .

Then

  • if N = 1 and l < , then u C loc 0 , β ( Ω ; R N ) , for some β ( 0 , 1 ) ,

  • if l = 0 , then u C loc 0 , β ( Ω ; R N ) , for every β ( 0 , 1 ) ,

  • if ω ( r ) C r α , for some α ( 0 , 1 ) and C > 0 , then u C loc 1 , γ ( Ω ; R N ) , for some γ ( 0 , 1 ) .

On the other hand, in the class of non-standard growth functionals, we also consider p ( x ) -growth functionals or functionals with variable exponent. A typical functional of this type is given as

P p ( x ) ( u ; Ω ) Ω D u p ( x ) d x .

These types of functionals are used to describe the behavior of strongly anisotropic materials. They appear in the study of non-Newtonian fluids that modify their viscosity when exists an electro-magnetic fluid [3,4,47]), or in image segmentation problems (see [36]).

Regularity results for p ( x ) -growth functionals are given by, for example, Cosica and Mingione [15], Acerbi and Mingione [14], and Eleuteri [28]. Recently, Baroni [5] obtained gradient continuity for related elliptic system: p ( x ) -Laplacian system.

For vector-valued case, we can expect partial regularity of minimizers for p ( x ) -energy-type functional:

p ( x ) ( u ; Ω ) Ω ( A i j α β ( x , u ) D α u i D β u j ) p ( x ) 2 d x ,

where ( A i j α β ( x , u ) ) is a positive definite symmetric tensor field on Ω × R N . About partial regularity results for this p ( x ) , see [44,46,49,51]. On the other hand, De Filippis [17] treated P p ( x ) under the condition that the images of maps are contained in a manifold and obtained partial regularity for a minimizer. For such manifold constrained case, if the images of maps are contained in a single coordinate chart, the functional is expressed as p ( x ) .

De Fillipis and Mingione [22] treated manifold constrained case also for P p , q and obtained partial regularity results.

The authors considered hybrid type of P p , q and P p ( x ) , double phase with variable exponents:

P p ( x ) , q ( x ) ( u ; Ω ) Ω ( D u p ( x ) + a ( x ) D u q ( x ) ) d x .

See [45,50].

In addition, we wish to recall the study carried out by Giannetti and Passarelli di Napoli in [30] where the authors consider the functional with variable exponent and log ; that is

P p ( x ) log x ( u ; Ω ) Ω D u p ( x ) log ( e + D u ) d x .

As they showed in [30], if p ( ) is logarithmic continuous, then a minimizer u is Hölder continuous, and Hölder continuity of p ( ) leads C 1 , α -regularity of u . From this article, we obtained many of the computational hints for cases involving logarithms and variable exponents.

In the present article, we treat P log with variable exponent p ( x ) . Let p ( x ) > 1 and a ( x ) 0 be bounded continuous functions defined on a bounded domain Ω R n . For x Ω and z R n N , we put

(1.2) F ( x , z ) z p ( x ) + a ( x ) z p ( x ) log ( e + z ) ,

and define a functional defined, for u : Ω R N , by

(1.3) ( u , Ω ) Ω F ( x , D u ) d x .

Let ω a ( ) and ω p ( ) modulus of continuity of a ( ) and p ( ) , respectively, namely

(1.4) a ( x ) a ( y ) ω a ( x y ) , p ( x ) p ( y ) ω p ( x y )

hold for every x , y Ω . We assume that ω a and ω p are bounded and satisfy

(1.5) limsup r 0 ω a ( r ) log 1 r = l a 0 , limsup r 0 ω p ( r ) log 1 r = l p 0 .

Also, we set

(1.6) p 0 inf x Ω p ( x ) , p 3 sup x Ω p ( x ) , a 3 sup x Ω a ( x ) .

We assume also that p 0 > 1 .

For the sake of simplicity, we assume that p 3 n . On the set D on which p ( ) > n , a minimizer u is automatically Hölder continuous by Sobolev’s imbedding theorem.

For B R ( y ) Ω , let us put

Data ( n , p 0 , p 3 , a 3 , sup B R ( y ) p ( x ) , inf B R ( y ) p ( x ) , sup 2 R t 0 ω a ( t ) , sup 2 R t 0 ω p ( t ) ) .

In what follows, for Lebesgue L p ( Ω ; R N ) and Sobolev spaces W k , p ( Ω ; R N ) , we omit the target space R N and simply write them as L p ( Ω ) and W k , p ( Ω ) .

Let us define local minimizers of as follows:

Definition 1.1

A function u W 1 , 1 ( Ω ) is called to be a local minimizer of if F ( , D u ) L 1 ( Ω ) and satisfies

( u ; supp φ ) ( u + φ ; supp φ ) ,

for any φ W loc 1 , 1 ( Ω ) with compact support in Ω .

For double phase functionals and functionals with variable exponents, or more generally, for non-autonomous variational problems, the regularity of weak solutions has been well studied in the last few years, after 2019. Just as examples we mention the study carried out by De Filippis, Mingione, Rădulescu, Repovš, and others. For non-standard growth problems see, for instance, the following articles: [10,16,2022,48,52] for double and multiple phase cases, [11,18] for p ( x ) -growth cases, and [19,20,2325,43] for more general cases.

Concerning further contributions to the regularity theory of double phase functionals we refer the reader to [43], that is an excellent survey in which we find important developments on problems with strong anisotropicity.

The main result of this article is the following:

Theorem 1.2

For a bounded domain Ω R n let a ( ) and p ( ) be functions defined on Ω satisfying (1.4) and (1.5) with l a = l s = 0 . Assume also that a ( ) 0 and that 1 < p 0 , p 3 < ( p 0 and p 3 are defined in (1.6)).

Let u W 1 , 1 ( Ω ) be a local minimizer of the functional

( u ) Ω ( D u p ( x ) + a ( x ) D u p ( x ) log ( e + D u ) ) d x .

Then, we have u C loc 0 , α ( Ω ) for any α ( 0 , 1 ) .

Moreover, when both a ( ) and p ( ) are Hölder continuous, then u C loc 1 , γ ( Ω ) for some γ ( 0 , 1 ) .

In order to prove the above theorem, we employ a freezing argument; namely we consider a frozen functional which is given by freezing the exponents and compare a minimizer of the original functional under consideration with that of frozen one.

Remark 1.3

Concerning the statement of the theorem by Baroni-Colombo-Mingione mentioned before and Theorem 1.2, the Hölder continuity of a minimizer u for some exponent can still be proven in the vectorial case N > 1, by requiring that la and lp in (1.5) are sufficiently small. See [4, Remark 3.3], which can be adapted to this situation. See also [5].

2 Zygmund spaces, definitions, and preparatory tools

In the sequel are useful the following properties of the logarithm function which are given in [7]. For x , y 0 and A , p > 1 , let us set

(2.1) log ( e + x y ) log ( e + x ) + log ( e + y ) ,

(2.2) log ( e + A x ) A log ( e + x ) ,

(2.3) ( x + y ) p log ( e + x + y ) ( 2 x ) p log ( e + 2 x ) + ( 2 y ) p log ( e + 2 y ) 2 p + 1 x p log ( e + x ) + 2 p + 1 y p log ( e + y ) .

For p 1 and α R , we define a Zygmund space L p log α L ( Ω ) and its norm by

L p log α L ( Ω ) f L 1 ( Ω ) ; Ω f p log α ( e + f ) < , f L p log α L inf λ > 0 ; Ω f λ p log α e + f λ d x 1 .

Iwaniec and Verde [38, Theorem 8.1] showed the following estimates:

f L p log L Ω f log e + f f L p ( Ω ) d x 1 p 2 f L p log L .

In [38, Theorem 8.1], they only consider α = 1 as exponent of log. It is clear that their proof is valid for any α 0 . Namely, we have

(2.4) f L p log α L Ω f p log α e + f f L p ( Ω ) d x 1 p 2 f L p log α L .

The following Hölder-type inequality holds (see, e.g., [37, (4.92)])

(2.5) f g L c log γ L C ( α , β , γ ) f L a log α L g L b log β L ,

whenever a , b , c > 1 and α , β , γ R satisfy

(2.6) 1 c = 1 a + 1 b , γ c = α a + β b .

By virtue of the above estimate, we can show the following lemma which will be useful in the later part.

Lemma 2.1

Assume that a , b , c , α , β , γ satisfy (2.6) and that f L a log α L ( B R ( y ) ) , where R ( 0 , 1 ) . Then, there exists a constant C = C ( α , β , γ , a , b , c , n ) for which the following estimate holds:

(2.7) B R ( y ) f c log γ ( e + f ) d x C f L c ( B R ( y ) ) c β b R c n b B R ( y ) f a log α ( e + f ) d x c a .

Proof

By (2.2), (2.4), and (2.5) with g = 1 , we have that

(2.8) B R ( y ) f c log γ ( e + f ) d x C f L c γ B R ( y ) f c log γ e + f f L c d x C f L c γ B R ( y ) f a log α e + f f L a d x c a B R ( y ) log β e + 1 1 L b d x c b ,

where we write simply L p ( p = a , b , c ) for L p ( B R ( y ) ) .

By (2.2), we can estimate the first integral of the right-hand side of (2.8) as

B R ( y ) f a log α e + f f L a d x c a 1 f L a α c a B R ( y ) f a log α ( e + f ) d x c a .

The second integral can be estimated as follows:

(2.9) B R ( y ) log β e + 1 1 L b d x c b C ( b , c , n ) R c n b log β c b e + 1 R ,

where we used (2.2) and the following fundamental fact:

log e + 1 R n b log e + 1 R n b = n b log e + 1 R .

Combining (2.8)–(2.9), we obtain

(2.10) B R ( y ) f c log γ ( e + f ) d x C ( a , b , c , n ) f L c γ f L a α c a R c n b log β c b e + 1 R B R ( y ) f a log α ( e + f ) d x c a .

Using “standard" Hölder inequality, we have that

f L c γ f L a α c a f L c γ ( C ( a , c , n ) R ( n a ) ( n c ) f L c ) α c a C ( a , c , α , γ , n ) R α c n ( a b ) f L c c β b .

Now, using this inequality and mentioning that

R α c n ( a b ) log β c b e + 1 R = R α n ( a β ) log e + 1 R β c b M ( 0 < R 1 )

holds for some constant M = M ( α , β , a , b , c , n ) , we obtain (2.7) from (2.10).□

3 Preliminary results

As in many articles on regularity theory for calculus of variations, we use the following lemmas.

Lemma 3.1

Let A , B , α be positive constants and β ( 0 , α ) . Then, for any γ < α , there exists a positive constant ε 0 = ε 0 ( α , β , γ , A ) with the following property: let us consider a non-negative and nondecreasing function Φ defined on [ 0 , R 0 ] for some R 0 > 0 satisfying, for ε ( 0 , ε 0 ) , the following inequality:

Φ A r R α + ε Φ ( R ) + B R β ,

for all 0 < r < R 0 . Then, for some positive constant c ( α , β , γ , A )

Φ ( r ) c ( α , β , γ , A ) r R γ Φ ( R ) + B r β

holds for any r ( 0 , R 0 ] .

Lemma 3.2

Let Φ : [ r 1 , r 2 ] [ 0 , ) be a bounded function. Assume that for r 1 s < t r 2 we have

Φ ( s ) θ Φ ( t ) + A ( t s ) γ + B

with A , B 0 and 0 θ < 1 . Then, there exists a positive constant c ( γ , θ ) depending only on γ and θ such that

Φ ( r 1 ) c ( γ , θ ) ( A ( r 2 r 1 ) γ + B ) .

For the proof of Lemma 3.1 see, for example, [32, Lemma 5.13] and for Lemma 3.2 see [35, p.191, Lemma 6.1].

For a constant p > 1 and γ [ 1 , p ) , let us put

(3.1) H ( x , ξ ) ξ p + a ( x ) ξ p log ( e + ξ ) ,

(3.2) H γ ( x , ξ ) ξ p γ + a γ ( x ) ξ p γ ( log ( e + ξ ) ) 1 γ , a γ ( x ) a 1 γ ( x ) .

Also, let us set

data ( n , p , sup x Ω a ( x ) , sup t 0 ω a ( t ) , l a ) .

We can obtain Sobolev-Poincaré inequality for H ( , ) , by modifying the proof of [12, Theorem 1.6].

First, we show the following proposition that correspond to [12, Proposition 3.1].

Proposition 3.3

Let a ( ) and ω a ( ) be as in (1.4) with (1.5), and H γ ( , ) be as (3.2) with p > 1 and γ [ 1 , p ) . Put ω 0 ω a ( e p n ) . Then, there exists a constant C 0 > 0 depending only ondataand l of (1.5), such that

(3.3) H γ ( x , ( f ) B R ( x ) ) C 0 [ 1 + ω 0 1 γ log 1 γ ( e + f L p γ ( B R ( x ) ) ) ] ( H γ ( , f ( ) ) ) B R ( x )

holds for any f L p ( B R ( x ) ) , where B R ( x ) R n is a ball with R e p n .

Proof

We can prove this proposition keeping in mind [12, Proposition 3.1]. Put

a γ , R ( x ) inf y B R ( x ) a γ ( y ) and H γ , R ( x , z ) z p γ + a γ , R ( x ) z p γ ( log ( e + z ) ) 1 γ .

Since H γ , R is convex, Jensen’s inequality gives

(3.4) H γ , R ( x , ( f ) B R ( x ) ) B R ( x ) H γ , R ( x , f ( y ) ) d y B R ( x ) H γ ( x , f ( y ) ) d y .

Now, we observe that

(3.5) H γ ( x , ( f ) B R ( x ) ) a γ ( x ) a γ , R ( x ) ( f ) B R ( x ) p γ log 1 γ ( e + ( f ) B R ( x ) ) + H γ , R ( x , ( f ) B R ( x ) ) ω a 1 γ ( R ) ( f B R ( x ) ) p γ log 1 γ ( e + ( f ) B R ( x ) ) + H γ , R ( x , ( f ) B R ( x ) ) .

Since, by Hölder’s inequality we have

( f ) B R ( x ) C ( n ) R n γ p f L p γ ( B R ( x ) )

for some positive constant C ( n ) depending only on n , taking R sufficiently small so that R n p e and using (2.1), we obtain

log ( e + ( f ) B R ( x ) ) log ( e + C ( n ) R n γ p f L p γ ( B R ( x ) ) ) log ( e + C ( n ) R n γ p ) + log ( e + f L p γ ( B R ( x ) ) ) log ( ( 1 + C ( n ) ) R n γ p ) + log ( e + f L p γ ( B R ( x ) ) ) .

Combining the above estimate with (3.5), we obtain, for some constant C ( γ ) depending only on γ , that

H γ ( x , ( f ) B R ( x ) ) C ( γ ) ω a ( R ) log ( 1 + C ( n ) ) + n γ p log 1 R 1 γ ( f ) B R ( x ) p γ + C ( γ ) [ ω a ( R ) log ( e + f L p γ ( B R ( x ) ) ) ] 1 γ ( f ) B R ( x ) p γ + H γ , R ( x , ( f ) B R ( x ) ) .

Now, mentioning condition (1.5) and combining the above estimate with (3.4), we obtain (3.3).□

Remark 3.4

In [12], Proposition 3.1 is corresponding to the above one for H ( x , z ) = z p + a ( x ) z q and is applied to H ¯ ( x , z ) = z p γ + [ a ( x ) ] 1 γ z q γ . This is possible since the Hölder continuity of a 1 γ ( ) is guaranteed by that of a ( ) . However, in our case we are supposing only logarithmic continuity on a ( ) pointing out that it does not imply the logarithmic continuity of a 1 γ ( ) . By such a reason, in this article, we show the above proposition for H γ directly.

In what follows, all radius R , r etc. are assumed to be smaller than e p n or e p 3 n . For the sake of convenience let us write for q > 1

r 0 ( q ) e q n .

Theorem 3.5

Let a ( ) and ω a be as in (1.4) with condition (1.5), and H ( , ) be as in (3.1) with p > 1 . Let μ L ( R n ) , μ 0 , and such that B R μ ( x ) d x = 1 , for B R Ω with R ( 0 , 1 ) . For μ and u L 1 ( B R ) , let us denote

u μ B R u ( x ) μ ( x ) d x .

Then, there exist exponents d 1 , d 2 : d 1 > 1 > d 2 depending only on n , p , such that

(3.6) B R H x , u u μ R d 1 d x 1 d 1 C B R [ H ( x , D u ) ] d 2 d x 1 d 2

holds, for every B R B R ( y ) Ω with R < r 0 ( p ) and u W 1 , 1 ( Ω , R N ) with [ H ( x , D u ) ] d 2 L loc 1 ( Ω ) . The constant C depends only ondata, sup μ , and D u L p ( B R ( x 0 ) ) .

Proof

Using (3.3), instead of [12, (3.1)], we can proceed as in the proof of [12, Theorem 1.6].

Step 1: Maximal estimate.

For bounded domain Ω R n and f L 1 ( Ω , R k ) , we define the restricted maximal operator:

(3.7) M ( f ) ( x ) M Ω ( f ) ( x ) sup B r ( x ) Ω , r < r 0 ( p ) B r ( x ) f ( y ) d y .

For 1 < p , 1 γ < p and f L p γ ( Ω ; R k ) , we have the following Hardy-Littlewood maximal inequality (of strong type):

(3.8) M ( f ) L p γ ( Ω ) C ( p , n ) f L p γ ( Ω ) .

We show the following estimate corresponding to [12, (3.4)], but for H γ , by the motivation stated in Remark 3.4. For γ ( 1 , p ) , let H γ be the function defined in (3.2). Then, we show the following estimate:

(3.9) Ω [ H γ ( x , M ( f ) ) ] d x C [ 1 + ω 0 1 γ log 1 γ ( e + f L p γ ( Ω ) ) ] Ω [ H γ ( x , f ) ] d x .

Let us set γ ( γ , p ) . Applying (3.3) for H γ on every B r ( x ) , taking supremum and mentioning the monotonicity of the function t H γ ( , t ) , we obtain

(3.10) H γ ( x , M ( f ) ( x ) ) C [ 1 + ω 0 1 γ log 1 γ ( e + f L p γ ( Ω ) ) ] M ( H γ ( , f ( ) ) ) ( x ) .

As in [12], integrating on Ω the γ γ th power of (3.10) and applying the Hardy-Littlewood maximal inequality (3.8) for H γ ( , f ) in L γ γ , we obtain that

(3.11) Ω [ H γ ( x , M ( f ) ( x ) ) ] γ γ d x C ( 1 + ω 0 1 γ log 1 γ ( e + f L p γ ) ) γ γ Ω [ M ( H γ ( , f ( ) ) ) ( x ) ] γ γ d x C ( 1 + ω 0 1 γ log 1 γ ( e + f L p γ ) ) Ω [ H γ ( x , f ( x ) ) ] γ γ d x .

Now, mentioning, as [12, (3.8)], that

(3.12) H γ ( x , z ) [ H γ ( x , z ) ] γ γ C ( γ , γ ) H γ ( x , z )

holds for some constant C ( γ , γ ) depending only on γ and γ , we obtain (3.9) from (3.11).

Step 2: A first Sobolev-Poincaré-type inequality.

Instead of [12, (3.10)], we prove

(3.13) B R H γ x , w w μ R n ( n 1 ) d x ( n 1 ) n C ( 1 + ω 0 1 γ log 1 γ ( e + D w L p γ ( B R ) ) ) B R H γ ( x , D w ) d x .

We can proceed as the second half of [12, p.456]. Instead of [12, (3.11)] we use the following generalized estimate:

w ˜ ( x ) w ( x ) w μ R C R B R D w ( y ) x y n 1 d y ,

which holds for almost all x Ω , and is shown by [39, Lemma 1.50] (see also the proof of [27, Theorem 7]). Then, as in [12, (3.12)], putting

D ˜ ( y ) D w ( y ) if y B R , 0 if y R n \ B R ,

we obtain, for any ε ( 0 , 1 ) , that

w ˜ c ε M 3 R ( D ˜ ) + c ε n 1 B 2 R ( x ) D ˜ ( y ) d y ,

where M 3 R is the maximal operator defined as (3.7) with Ω = B 3 R ( x ) . On the other hand, by virtue of (2.3), we see that [12, (3.13)] holds also for H γ replacing both p and q with p γ . Taking p = q and using (3.3), instead of [12, (3.1)], we can proceed as in [12, p. 457] and obtain (3.13).

Step 3: Improved Sobolev-Poincaré inequality. Let us choose γ ( 1 , p ) in definition (3.2) of H γ , so that 1 < γ < n ( n 1 ) and let us put

d 1 n γ ( n 1 ) ( > 1 by the above choice of γ ) .

Then, as [12, p. 458], recalling (3.12), we obtain

B R H x , w w μ R d 1 d x 1 d 1 C B R H γ x , w w μ R n ( n 1 ) d x γ ( n 1 ) n C ( 1 + ω 0 1 γ log 1 γ ( e + D w L p γ ( B R ) ) ) γ B R H γ ( x , D w ) d x 1 γ C ( 1 + ω 0 log ( e + D w L p γ ( B R ) ) ) B R ( H ( x , D w ) ) 1 γ d x 1 γ .

Thus, we obtain (3.6) for d 1 = n γ ( n 1 ) > 1 and d 2 = 1 γ < 1 for any γ ( 1 , n ( n 1 ) ) .□

Corollary 3.6

Suppose that all conditions on H ( , ) are satisfied. Then

  1. there exist exponents d 1 , d 2 : d 1 > 1 > d 2 and exists a constant C depending only ondata, d 1 and d 2 , such that

    B R H x , u ( u ) B R R d 1 d x 1 d 1 C B R [ H ( x , D u ) ] d 2 d x 1 d 2 ,

    holds for any B R = B R ( y ) Ω with R < r 0 ( p ) and u W 1 , 1 ( Ω , R N ) with H ( , D u ( ) ) d 2 L 1 ( Ω ) . Here, and in what follows, we denote

    ( u ) B R B R u ( x ) d x 1 B R B R u ( x ) d x .

  2. Let D be a subset of B R having positive measure. Then, there exists a constant C depending only ondata, R n D , and D u L p ( B R ) and exponents d 1 , d 2 : d 1 > 1 > d 2 depending only ondatasuch that the following inequality holds whenever u W 1 , 1 ( B R ) with H ( , D u ( ) ) L 1 ( Ω ) satisfying u 0 on D :

    B R H x , u R d 1 d x 1 d 1 C B R [ H ( x , D u ) ] d 2 d x 1 d 2 .

Proof

In Theorem 3.5, choosing μ ( x ) B R 1 χ B R , we obtain assertion (i). If we choose,

μ ( x ) = 0 x B R \ D , 1 D x D ,

we obtain assertion (ii).□

For any y Ω and R > 0 such that B R ( y ) Ω , let us put

p 2 ( y , R ) sup B R ( y ) p ( x ) , p 1 ( y , R ) inf B R ( y ) p ( x ) .

Lemma 3.7

(Caccioppoli-type inequality) Let be the functional defined by (1.2) and (1.3) with p ( ) > 1 and a ( ) 0 satisfying (1.4) and (1.5), and let u W 1 , 1 ( Ω , R N ) be a local minimizer of the functional . Then, there are positive constants R 0 and C ( 3.14 ) , depending only onData, such that

(3.14) B r 1 ( y ) F ( x , D u ) d x C ( 3.14 ) ( r 2 r 1 ) p 1 ( y , r 2 ) p 2 ( y , r 2 ) B r 2 ( y ) F x , u k r 2 r 1 d x

holds for any k R N , 0 < r 1 < r 2 R < R 0 with B R ( y ) Ω .

Proof

Let us choose a positive constant R 0 such that

(3.15) ω p ( 2 R 0 ) < p 0 2 n p 0 .

Then, for any B R ( y ) Ω with 0 < R < R 0 , we have

(3.16) p 2 ( y , R ) < p 1 ( y , R ) n p 1 ( y , R ) n p 1 ( y , R ) .

For any B R ( y ) with 0 < R < R 0 , and s , t such that 0 < r 1 s < t r 2 R , let η be a cutoff function such that η 1 on B s ( y ) , η 0 outside B t ( y ) and D η 2 t s . For a constant vector k R N , let us put w u η ( u k ) . Since

D w = ( 1 η ) D u ( u k ) D η ,

using (2.3), we have

F ( x , D w ) c 0 [ ( ( 1 η ) D u ) p ( x ) + ( u k D η ) p ( x ) ] + c 0 a ( x ) [ ( ( 1 η ) D u ) p ( x ) × log ( e + ( 1 η ) D u ) + ( u k D η ) p ( x ) log ( e + u k D η ) ] ,

where c 0 is a constant depending only on p 3 . Since we are assuming that u is a local minimizer of , the integrability of F ( , D u ) on B R ( y ) is assumed implicitly. So, D u p ( x ) is integrable and we have

u W 1 , p ( x ) ( B R ( y ) ) W 1 , p 1 ( y , R ) ( B R ( y ) ) L p 1 ( y , R ) ( B R ( y ) ) ,

and that

( u k D η ) p ( x ) log ( e + u k D η ) L 1 ( B R ( y ) )

by virtue of (3.16). Therefore, F ( x , D w ) L 1 ( B R ( y ) ) .

Then, by the minimality of u , we have

B s ( y ) F ( x , D u ) d x B t ( y ) F ( x , D u ) d x B t ( y ) F ( x , D w ) d x c 0 B t ( y ) ( 1 η ) p ( x ) D u p ( x ) ( 1 + a ( x ) log ( e + ( 1 η ) D u ) ) d x + c 0 B t ( y ) u k t s p ( x ) 1 + a ( x ) log e + u k t s d x c 0 B t ( y ) \ B s ( y ) F ( x , D u ) d x + c 0 B t ( y ) u k t s p ( x ) 1 + a ( x ) log e + u k t s d x .

Now we can use the hole-filling method. Add c 0 B s ( y ) F ( x , D u ) d x to the both sides and divide them by c 0 + 1 , then, using (2.2), we obtain

B s ( y ) F ( x , D u ) d x c 0 c 0 + 1 B t ( y ) F ( x , D u ) d x + B t ( y ) u k t s p ( x ) 1 + a ( x ) log e + u k t s d x c 0 c 0 + 1 B t ( y ) F ( x , D u ) d x + r 2 r 1 ( t s ) p 2 ( y , r 2 ) + 1 B t ( y ) u k p ( x ) 1 + a ( x ) log e + u k r 2 r 1 d x .

From the above estimate, using Lemma 3.2 with

Φ ( t ) = B t ( y ) F ( x , D u ) d x , γ = p 2 ( y , r 2 ) + 1 , A = ( r 2 r 1 ) B r 2 u k p ( x ) 1 + a ( x ) log e + u k r 2 r 1 d x , B = 0

and mentioning that 0 < r 2 r 1 < 1 , we obtain

B r 1 ( y ) F ( x , D u ) d x C 1 ( r 2 r 1 ) p 2 ( y , r 2 ) B r 2 ( y ) u k p ( x ) 1 + a ( x ) log e + u k r 2 r 1 d x C ( r 2 r 1 ) p 1 ( y , r 2 ) ( r 2 r 1 ) p 2 ( y , r 2 ) B r 2 ( y ) 1 ( r 2 r 1 ) p 1 ( r 2 ) u k p ( x ) 1 + a ( x ) log e + u k r 2 r 1 d x C ( r 2 r 1 ) p 1 ( y , r 2 ) p 2 ( y , r 2 ) B r 2 ( y ) u k r 2 r 1 p ( x ) 1 + a ( x ) log e + u k r 2 r 1 d x .

Thus, we reach the goal, that is, (3.14).□

In what follows, R 0 denotes the positive constant that satisfies (3.15).

Proposition 3.8

Let u W loc 1 , 1 ( Ω ) with F ( x , D u ) L loc 1 ( Ω ; R N ) be a local minimizer of . Then, for any compact subset K Ω , we have F ( x , D u ) L 1 + δ 0 ( K ) and there exist positive constants R 1 , δ 0 , and C depending only ondataand K, such that

(3.17) B R 2 ( y ) F ( x , D u ) 1 + δ 0 d x 1 1 + δ 0 C + C B R ( y ) F ( x , D u ) d x

holds for any B R ( y ) K with R ( 0 , R 1 ) .

Proof

For K Ω let d 0 dist ( K , Ω ) and K { x Ω ; dist ( x , K ) d 0 2 } . In the following part of the proof, we always assume that R < R 1 min { d 0 4 , R 0 } .

By the assumption (1.5) on p ( x ) , R p 1 ( R ) p 2 ( R ) is bounded. So, for any y K Ω , by Lemma 3.7, we have

(3.18) B R 2 ( y ) F ( x , D u ) d x C B R ( y ) F x , u ( u ) R R d x ,

where C depends only on C ( 3.14 ) and l p of (1.5). Let us put

U R u ( u ) R R .

Then, we can write

(3.19) B R ( y ) F x , u ( u ) R R d x = B R ( y ) [ U R p ( x ) + a ( x ) U R p ( x ) log ( e + U R ) ] d x .

Let p 2 = p 2 ( y , R ) . Fixing

a ˜ ( x ) ( a ( x ) ) p 2 p ( x ) ,

since

a ( x ) U R p ( x ) a ˜ ( x ) U R p 2 ( a ( x ) 1 p ( x ) U R 1 ) , 1 ( 1 > a ( x ) 1 p ( x ) U R 0 ) ,

we have

(3.20) a ( x ) U R p ( x ) log ( e + U R ) log ( e + U R ) ( 1 + a ˜ ( x ) U R p 2 ) .

On the other hand, since log ( e + t ) 1 + t for t 0 , we have that log ( e + U R ) 2 + U R p 2 . So, from (3.20), we obtain

(3.21) a ( x ) U R p ( x ) log ( e + U R ) 2 + U R p 2 + a ˜ ( x ) log ( e + U R ) U R p 2 .

Writing

H ˜ p 2 ( x , z ) z p 2 + a ˜ ( x ) z p 2 log ( e + z ) ,

combining (3.18), (3.19), and (3.21) and using Theorem 3.5 for H ˜ p 2 , we obtain

(3.22) B R 2 ( y ) F ( x , D u ) d x C + C B R ( y ) H ˜ p 2 x , u ( u ) R R d x C + C B R ( y ) H ˜ p 2 ( x , D u ) d 2 d x 1 d 2 .

Let us estimate the last integral in (3.22). By virtue of the continuity of p ( ) , for θ ( d 2 , 1 ) , we can take R > 0 sufficiently small so that p 2 d 2 θ p 1 , where p 1 p 1 ( y , R ) . Then, for the first term of H ˜ p 2 , by Hölder’s inequality, we can see that

(3.23) B R ( y ) D u p 2 d 2 d x 1 d 2 B R ( y ) D u θ p 1 p 2 θ p 1 = B R ( y ) D u θ p 1 ( p 2 p 1 ) θ p 1 B R ( y ) D u θ p 1 1 θ I I I .

Without loss in generality, we assume that ( p 2 p 1 ) θ p 1 1 . Then, by assumption (1.5) on p , we can estimate I as follows:

I C ( n ) ( R p 2 ( R ) + p 1 ( R ) ) n θ p 1 B R ( y ) D u θ p 1 d x ( p 2 p 1 ) θ p 1 C ( n , l p ) ( 1 + R n + ( u ; K ) ) .

So, we can estimate I by some constant depending only on n , l p , ( u ; K ) .

On the other hand, for I I , since p 1 p ( x ) , we have that

I I C + C B R ( y ) D u θ p ( x ) d x 1 θ .

Combining these estimates with (3.23), we obtain

(3.24) B R ( y ) D u p 2 d 2 d x 1 d 2 C + C B R ( y ) D u θ p ( x ) d x 1 θ .

Also, for the second term of H ˜ p 2 , by Hölder’s inequality, we obtain that

B R ( y ) ( a ˜ ( x ) D u p 2 log ( e + D u ) ) d 2 d x 1 d 2 B R ( y ) ( a ˜ ( x ) D u p 2 log ( e + D u ) ) d 2 θ p 1 d 2 p 2 d x 1 d 2 d 2 p 2 θ p 1 = B R ( y ) a θ p 1 p ( x ) D u θ p 1 ( log ( e + D u ) ) θ p 1 p 2 d x p 2 θ p 1 C B R ( y ) ( ( log ( e + D u ) ) θ + ( a ( x ) D u p ( x ) log ( e + D u ) ) θ ) d x p 2 θ p 1 .

Here, for the last inequality we used the following facts:

log ( e + D u ) θ p 1 p 2 log ( e + D u ) θ , since log ( e + D u ) 1 and p 1 p 2 1 , a θ p 1 p ( x ) D u θ p 1 1 + a θ D u θ p ( x ) , since p ( x ) p 1 .

Now, mentioning that log ( e + D u ) 1 + D u p ( x ) , we can proceed as we deduced (3.24) from (3.23) and achieve

(3.25) B R ( y ) ( a ˜ ( x ) D u p 2 log ( e + D u ) ) d 2 d x 1 d 2 C 1 + B R ( y ) D u θ p ( x ) d x + B R ( y ) ( a ( x ) D u p ( x ) log ( e + D u ) ) θ d x 1 θ .

Combining (3.22), (3.24), and (3.25), we obtain the following estimate:

B R 2 ( y ) F ( x , D u ) d x C B R ( y ) F ( x , D u ) θ d x 1 θ + C .

Now, by virtue of the so-called reverse Hölder inequality with increasing support or Gehring-type inequality (see, for example, [34, p. 299 Theorem 3]), we obtain the assertion.□

Also, we need higher integrability results on the neighborhood of the boundary for a minimizer of ( u ) H ( x , D u ) d x . Let us use the following notation: for T > 0 we put

B T B T ( 0 ) , B T + { x R n ; x < T , x n > 0 } , Γ T { x R n ; x < T , x n = 0 } .

We say “ f = g on Γ T " when, for any η C 0 ( B T ) , we have ( f g ) η W 0 1 , 1 ( B T + ) . Let y B T , we write

Ω r B r ( y ) B T + .

We prove the following proposition on the higher integrability near the boundary.

Proposition 3.9

Let p be constant, p > 1 , and a ( x ) a non-negative function defined on B T + satisfying (1.4) with (1.5). For H ( s , ξ ) defined by (3.1) and A B T + , let be a functional given by

( w ; A ) A H ( x , D w ) d x ,

for w : B T + R n . Let v W 1 , p ( B T + ) be a local minimizer of in the class

{ w W 1 , p ( B T + ) ; w = u on Γ T } ,

where u W 1 , p ( B T + ) is a given function such that

B T + ( H ( x , D u ) ) 1 + δ 0 d x <

for some δ 0 > 0 . Then, for any S ( 0 , T ) , there exist two constants δ ( 0 , δ 0 ) and C > 0 such that for any y B S + and 0 < R < 1 2 min { T S , R 0 } we have

Ω R 2 ( H ( x , D v ) ) 1 + δ d x 1 1 + δ C Ω R H ( x , D v ) d x + C Ω R ( H ( x , D u ) ) 1 + δ d x 1 1 + δ .

Proof

For convenience, we extend v , u , D v , D u to be zero in B T \ B T + . Also, we extend a ( x ) by its even extension. Of course, because of extended v , u may have discontinuity on Γ T , they are not always in W loc 1 , 1 ( B T ) , and, therefore, D v , D u do not necessarily coincide with distributional derivatives of v , u on B T . On the other hand, since v u = 0 on Γ T , the extended v u is in the class W 1 , p ( B T ) and D v D u can be regarded as the weak derivatives of v u in B T .

Now, let us fix x 0 B S + arbitrarily and consider Ω R ( x 0 ) , for R < min { R 0 , T S } 2 . In what follows, we abbreviate as follows:

(3.26) p i p i ( x 0 , 2 R ) ( i = 1 , 2 ) .

Let R be a positive constant satisfying R ( T S ) 2 . For x 0 B S + , we treat the two cases x 0 n 3 4 R and x 0 n > 3 4 R separately.

Case 1. Suppose that x 0 n 3 4 R . Take radii s , t so that 0 < R 2 s < t R and choose a cutoff function η C 0 ( B T ) such that 0 η 1 , η 1 on B s , supp η B t and D η 2 ( t s ) . Defining

φ η ( v u ) ,

we have φ W 0 1 , 1 ( B T + ) with supp φ B s , and the following development

D ( v φ ) = ( 1 η ) D v ( v u ) D η + η D u .

Then, by virtue of the minimality of v , for R 2 r 1 s < t r 2 R , we have

Ω s H ( x , D v ) d x Ω t H ( x , D v ) d x Ω t H ( x , D ( v φ ) ) d x Ω t ( D ( v φ ) p + a ( x ) D ( v φ ) p log ( e + D ( v φ ) ) ) d x c 1 ( p ) Ω t \ Ω s H ( x , D v ) + Ω t H ( x , D u ) d x + c 1 ( p ) Ω t v u t s p + a ( x ) r 2 r 1 t s v u t s p log e + v u r 2 r 1 d x .

Here, in the last inequality, we used (2.2) and (2.3).

Now, we use the hole filling method as in the proof of Proposition 3.8. Namely, adding

c 1 Ω s H ( x , D v ) d x

to both sides and dividing by c 1 + 1 in the same both sides, we obtain

Ω s H ( x , D v ) d x θ Ω t H ( x , D v ) d x + Ω t H ( x , D u ) d x + r 2 r 1 ( t s ) p + 1 Ω t v u p + a ( x ) v u p log e + v u r 2 r 1 d x ,

where we put θ = c 1 ( c 1 + 1 ) ( 0 , 1 ) and use (2.2).

Applying Lemma 3.2, we have that there exists a constant C depending only on θ and p , such that

Ω ρ H ( x , D v ) d x C r 2 r 1 ( R ρ ) p + 1 Ω R v u p + a ( x ) v u p log e + v u r 2 r 1 d x C Ω R H ( x , D u ) d x .

Taking r 2 = R , r 1 = ρ = R 2 in the above estimate, and using Corollary 3.6 (ii) and (2.3), we obtain

(3.27) Ω R 2 H ( x , D v ) d x C 1 R p Ω R v u p + a ( x ) v u p log e + 2 v u R d x + C Ω R H ( x , D u ) d x . C Ω R H x , v u R d x + C Ω R H ( x , D u ) d x C Ω R H ( x , D v ) d 2 d x 1 d 2 + C Ω R H ( x , D u ) d 2 d x 1 d 2 + C Ω R H ( x , D u ) d x C Ω R H ( x , D v ) d 2 d x 1 d 2 + C Ω R H ( x , D u ) d x ,

where d 2 ( 0 , 1 ) is the same constant that appears in Corollary 3.6 (ii).

Case 2. Let us deal with the case that x 0 n > 3 4 R . Replacing u with the integral mean ( v ) 3 R 4 = B 3 R 4 ( x 0 ) v d x , and modifying radii suitably, we can proceed as in Case 1, and obtain for some constant C , depending on given data and ( v ; B T + ) , we have

Ω R 2 H ( x , D v ) d x = B R 2 H ( x , D v ) d x C B 3 R 4 ( H ( x , D v ) ) d 2 d x 1 d 2 .

Thus, changing the constants if necessary, we see that (3.27) holds for every 0 < R < min { R 0 , ( S T ) 2 } . Since we are assuming that H ( x , D u ) L 1 + δ 0 , the reverse Hölder inequality due to [33] allows us to obtain the assertion, for some δ min { δ 0 , δ 2 } .□

By virtue of Proposition 3.8 (with p ( x ) p ) and Proposition 3.9, we have the following global higher integrability for functions which minimize with Dirichlet boundary condition.

Corollary 3.10

Let p and a ( x ) be as in Proposition3.9. Assume that u W 1 , p ( B R ) satisfies

B R ( H ( x , D u ) ) 1 + δ 0 d x < ,

for some constant δ 0 ( 0 , 1 ) . Let v W 1 , p ( B R ) be a minimizer of

( w , B R ) B R H ( x , D w ) d x

in the class

u + W 0 1 , p ( B R ) = { w W 1 , p ( B R ) ; u w W 0 1 , p ( B R ) } .

Then, there exist positive constants δ < δ 0 and C such that we have H ( x , D v ) L 1 + δ ( B R ) and

(3.28) B R ( H ( x , D v ) ) 1 + δ d x C B R ( H ( x , D u ) ) d x 1 + δ .

Proof

By virtue of Propositions 3.8 and 3.9, using covering argument and flattening every piece of B R , we can choose a constant δ ( 0 , δ 0 ) so that

B R ( H ( x , D v ) ) 1 + δ d x 1 1 + δ C B R H ( x , D v ) d x + C B R ( H ( x , D u ) ) 1 + δ d x 1 1 + δ

holds, and then, by the minimality of v , we have

B R ( H ( x , D v ) ) 1 + δ d x 1 1 + δ C B R H ( x , D u ) d x + C B R ( H ( x , D u ) ) 1 + δ d x 1 1 + δ .

Using Hölder inequality for the first term of the right-hand side that gives us the assertion.□

Remark 3.11

By the Hölder inequality, we can see that the assertions of Proposition 3.8, 3.9, and Corollary 3.10 remain valid even if the positive numbers δ 0 (in Proposition 3.8) or δ are replaced by smaller one.

4 Proof of the main theorem

In this section we prove Theorem 1.2. We employ the so-called direct approach, namely we consider a frozen functional for which the regularity theory has been established in [12] and compare a local minimizer of the frozen functional with u under consideration.

Proof of Theorem 1.2

Let K and R 1 be as in Proposition 3.8, x 0 K an arbitrarily fixed point.

For B R ( y ) such that B 2 R ( y ) B R 1 ( x 0 ) , putting p i as (3.26), we define a frozen functional R as

(4.1) F R ( x , z ) z p 2 + a ( x ) p 2 p ( x ) z p 2 log ( e + z ) ,

(4.2) R ( w , D ) = B R ( y ) F R ( x , D w ) d x .

In what follows, let us abbreviate

a ¯ ( x ) = ( a ( x ) ) 1 p ( x ) ( = a ˜ 1 p 2 ( x ) ) .

For ( x , t ) Ω × [ 0 , ) , let us set

f R ( x , t ) t p 2 + a ¯ ( x ) t p 2 log ( e + t ) , f R ( x , t ) f R t ( x , t ) , f R ( x , t ) 2 f R t 2 ( x , t ) .

It is easy to see that

f R ( x , t ) t f R ( x , t ) t 2 f R ( x , t ) .

Let us define the auxiliary vector field V f R : Ω × R n N R n N as

V f R ( x , ξ ) f R ( x , ξ ) ξ 1 2 ξ .

As in [29, Lemma 2.2], we see that, for every x Ω and for all ξ , η R n N ,

(4.3) f R ( x , ξ ) ξ ξ f R ( x , η ) η η , ξ η V f R ( x , ξ ) V f R ( x , η ) 2

(4.4) ξ η 2 f R ( x , ξ + η ) .

We divide the rest part of the proof into two parts. We prove the Hölder continuity of u in Part 1 and of the gradient D u in Part 2.

Part 1. Let v W p 2 ( B R ( y ) ) be a minimizer of R in the class

u + W 0 p 2 ( B R ( y ) ) { w W p 2 ( B R ( y ) ) ; w u W 0 p 2 ( B R ( y ) ) } .

Let us put the modulus of continuity of a p 2 p ( x ) ( x ) as ω ˆ a . Remarking that p 2 p ( x ) 1 and p ( x ) > 1 , from (1.5) with l a = l p = 0 we can deduce that

lim r 0 ω ˆ a ( r ) log 1 r = 0 .

So, we can apply (5.21) of [7] for v to see that there exists a constant C depending on n , p 2 , D v L p 2 ( B R ( y ) ) and γ such that the decay estimate

(4.5) B ρ ( y ) F R ( x , D v ) d x C ρ R n γ B R ( y ) F R ( x , D v ) d x C ρ R n γ B R ( y ) F R ( x , D u ) d x

holds.

Here, we mention that by the coercivity of the functional and the minimality of v we have the following:

D v L p 2 ( B R ( y ) ) p 2 R ( v , B R ( y ) ) R ( u , B R ( y ) ) .

Let us take R > 0 sufficiently small so that ω p ( 2 R ) < p 1 ( 1 + δ 0 ) . Then, we have

p 2 p 1 + ω p ( 2 R ) < p 1 ( 1 + δ 0 ) p ( x ) ( 1 + δ 0 ) for all x B 2 R ( y ) ,

and therefore, there exists a constant C ( p 2 ) > 0 such that

F R ( x , ξ ) C ( p 2 ) ( 1 + F ( x , ξ ) ) 1 + δ 0

holds for any ( x , ξ ) B R ( y ) × R n N . Now, by virtue of above two estimates and Proposition 3.8, we can see, for a constant C > 0 depending only on the given data on the functional, that

D v L p 2 ( B R ( y ) ) p 2 R ( v , B R ( y ) ) C ( 1 + ( u , K ) ) 1 + δ 0 .

Because of the local minimality of u , the last quantity is finite. Consequently, we can regard the constant in (4.5) as depending only on given data and ( u , K ) .

For further convenience, let us mention that, from (4.5), we have

(4.6) B ρ ( y ) ( 1 + F R ( x , D v ) ) d x C ρ R n γ B R ( y ) ( 1 + F R ( x , D v ) ) d x C ρ R n γ B R ( y ) ( 1 + F R ( x , D u ) ) d x .

Using (4.4), we obtain

(4.7) B ρ ( y ) ( 1 + F R ( x , D u ) ) d x C B ρ ( y ) ( 1 + V f R ( x , D u ) 2 ) d x C B ρ ( y ) V f R ( x , D u ) V f R ( x , D v ) 2 d x + C B ρ ( y ) ( 1 + V f R ( x , D v ) 2 ) d x C B ρ ( y ) D u D v 2 f R ( x , D u + D v ) d x + C B ρ ( y ) ( 1 + F R ( x , D v ) ) d x I + I I

Since the second integral I I is estimated as (4.6), it is enough to estimate the first integral I . For I , as [31, (3.10)], we have that

B R ( y ) D u D v 2 f R ( x , D u + D v ) d x C ( R ( u , B R ( y ) ) R ( v , B R ( y ) ) ) .

So, mentioning that f R 0 and using the minimality of u for , we can estimate I as

(4.8) I B R ( y ) D u D v 2 f R ( x , D u + D v ) d x C ( R ( u , B R ( y ) ) R ( v , B R ( y ) ) ) C [ R ( u , B R ( y ) ) ( u , B R ( y ) ) ] + C [ ( v , B R ( y ) ) R ( v , B R ( y ) ) ] .

In order to estimate the first term of the above last line, let us divide it as follows:

(4.9) R ( u , B R ( y ) ) ( u , B R ( y ) ) B R ( y ) D u p 2 D u p ( x ) d x + B R ( y ) ( ( a ¯ ( x ) D u ) p 2 ( a ¯ ( x ) D u ) p ( x ) log ( e + D u ) ) d x I I I + I V .

For t 0 and q > p > 1 , by Lagrange’s mean value theorem and a direct calculation, it is easy to see that

(4.10) t q t p q p t q θ + ( 1 θ ) p log t ( for some ) θ ( 0 , 1 ) q p t q log ( e + t ) ( t 1 ) q p t log t q p 1 e ( t ( 0 , 1 ) ) q p ( 1 + t q ) log ( e + t ) .

Using (4.10), we can estimate I I I as

I I I C ω p ( 2 R ) B R ( y ) ( 1 + D u p 2 ) log ( e + D u ) d x C ω p ( 2 R ) B R ( y ) log ( e + D u ) d x + B R ( y ) D u p 2 log ( e + D u ) d x .

Let ε ( 0 , 1 ) be a constant which is specified later. In order to estimate the second integral of the right-hand side in the above inequality, we use Lemma 2.1 for

f = D u , g 1 , c = p 2 , a = ( 1 + ε ) p 2 , b = p 2 ( 1 + ε ) ε , γ = 1 , α = 0 , β = 1 + ε ε ,

and obtain

(4.11) I I I C ω p ( 2 R ) B R ( y ) D u d x + C ω p ( 2 R ) D u L p 2 ( B R ( y ) ) R ε n 1 + ε B R ( y ) D u ( 1 + ε ) p 2 d x 1 1 + ε .

For I V , using (4.10), we can proceed in a similar way as in [30] and obtain

(4.12) I V ω p ( 2 R ) B R ( y ) ( 1 + ( a ¯ D u ) p 2 ) log ( e + a ¯ D u ) log ( e + D u ) d x = ω p ( 2 R ) B R ( y ) log ( e + a ¯ D u ) log ( e + D u ) d x + B R ( y ) ( a ¯ D u ) p 2 log ( e + a ¯ D u ) log ( e + D u ) d x ω p ( 2 R ) ( I V 1 + I V 2 ) .

Using (2.2), we estimate I V 1 as

(4.13) I V 1 sup a ¯ B R ( y ) log 2 ( e + D u ) d x C sup a ¯ B R ( y ) ( 1 + D u ) d x .

By (2.1), when a ¯ 0 , we gain that

log ( e + D u ) = log e + 1 a ¯ a ¯ D u log e + 1 a ¯ + log ( e + a ¯ D u ) .

Using this inequality and Lemma 2.1 for

c = p 2 , a = ( 1 + ε ) p 2 , b = p 2 ( 1 + ε ) ε , γ = 2 , α = 1 + ε , β = 1 + ε ε ,

we can estimate I V 2 as follows:

(4.14) I V 2 B R ( y ) ( a ¯ D u ) p 2 log ( e + a ¯ D u ) log ( e + a ¯ D u ) + log e + 1 a ¯ d x B R ( y ) 3 2 ( a ¯ D u ) p 2 log 2 ( e + a ¯ D u ) + ( a ¯ D u ) p 2 log 2 e + 1 a ¯ d x B R ( y ) 3 2 ( a ¯ D u ) p 2 log 2 ( e + a ¯ D u ) d x + C sup a ¯ p 2 B R ( y ) D u p 2 d x C D u L p 2 ( B R ( y ) ) R ε n ( 1 + ε ) B R ( y ) ( a ¯ D u ) p 2 ( 1 + ε ) log 1 + ε ( e + a ¯ D u ) d x 1 ( 1 + ε ) + C sup a ¯ p 2 B R ( y ) D u p 2 d x ,

where, for the third inequality, we observe that lim t 0 t log 2 e + 1 t = 0 .

Combining (4.9), (4.11), (4.12), (4.13), and (4.14), we obtain

(4.15) R ( u , B R ( y ) ) ( u , B R ( y ) ) C ω p ( 2 R ) D u L p 2 ( B R ( y ) ) R ε n 1 + ε B R ( y ) D u ( 1 + ε ) p 2 d x 1 1 + ε + B R ( y ) ( a ¯ D u ) p 2 ( 1 + ε ) log 1 + ε ( e + a ¯ D u ) d x 1 1 + ε + C ω p ( 2 R ) ( 1 + sup a ¯ ) B R ( y ) ( 1 + D u ) d x C ω p ( 2 R ) D u L p 2 ( B R ( y ) ) R ε n 1 + ε B R ( y ) D u ( 1 + ε ) p 2 d x 1 1 + ε + B R ( y ) ( a ¯ D u ) p 2 ( 1 + ε ) log 1 + ε ( e + a ¯ D u ) d x 1 1 + ε + C ω p ( 2 R ) R n + B R ( y ) D u p 2 d x .

Now, let δ 0 be as in Proposition 3.8, and choose positive constants ε and R sufficiently small such that ε < δ 0 4 and ω p ( 4 R ) < δ 0 8 . Mention also that, without loss in generality, we can assume that ( 1 + δ 0 4 ) p 0 2 . Then we have

1 + δ 0 4 p 2 ( 2 R ) 1 + δ 0 4 ( p 1 ( 2 R ) + ω p ( 4 R ) ) 1 + δ 0 4 p 1 ( 2 R ) + 1 p 1 ( 2 R ) p 1 ( 2 R ) ω p ( 4 R ) 1 + δ 0 4 + 2 ω p ( 4 R ) p 1 ( 2 R ) 1 + δ 0 4 + 2 ω p ( 4 R ) p ( x ) 1 + δ 0 2 p ( x ) ,

for all x B 2 R . We can estimate the first integral of the right-hand side in (4.15) as

(4.16) R n ε 1 + ε B R ( y ) D u p 2 ( 1 + ε ) d x 1 1 + ε = c ( n ) R n B R ( y ) D u p 2 ( 1 + ε ) d x 1 1 + ε C R n B R ( y ) D u p 2 ( 1 + δ 0 4 ) d x 1 1 + δ 0 4 C R n B R ( y ) ( 1 + D u ) p 1 ( 1 + δ 0 4 + 2 ω p ( 4 R ) ) d x 1 1 + δ 0 4 C R n B R ( y ) ( 1 + D u ) p ( x ) ( 1 + δ 0 4 + 2 ω p ( 4 R ) ) d x 1 1 + δ 0 4 C R n + C R n B R ( y ) F ( x , D u ) 1 + δ 0 4 + 2 ω p ( 4 R ) d x 1 1 + δ 0 4 .

For the last inequality we used Assumption (1.5) on ω p . We mention that in the last line the second constant C depends also on K F ( x , D u ) d x . Similarly, we can estimate the second integral of the right-hand side in (4.15) as

(4.17) R n ε 1 + ε B R ( y ) ( a ¯ D u ) p 2 ( 1 + ε ) log 1 + ε ( e + a ¯ D u ) d x 1 1 + ε = c ( n ) R n B R ( y ) ( a ¯ D u ) p 2 ( 1 + ε ) log 1 + ε ( e + a ¯ D u ) d x 1 1 + ε C R n B R ( y ) ( a ¯ D u ) p 2 ( 1 + δ 0 4 ) log 1 1 + δ 0 4 ( e + a ¯ D u ) d x 1 1 + δ 0 4 R n B R ( y ) a ¯ D u p 2 ( 1 + δ 0 4 ) c ( δ 0 , sup a ¯ ) + log 1 + δ 0 4 ( e + D u ) d x 1 1 + δ 0 4 ( by (2.1) ) C R n B R ( y ) D u p 2 ( 1 + δ 0 4 ) + a ¯ D u p 2 ( 1 + δ 0 4 ) log 1 + δ 0 4 ( e + D u ) d x 1 1 + δ 0 4 C R n B R ( y ) 1 + D u p 1 ( 1 + δ 0 4 + 2 ω p ( 4 R ) ) + a ¯ D u p 1 1 + δ 0 4 + 2 ω p ( 4 R ) log 1 + δ 0 4 + 2 ω p ( 4 R ) ( e + D u ) d x 1 1 + δ 0 4 C R n + C R n B 2 R ( y ) ( D u p ( x ) + a ¯ D u p ( x ) log ( e + D u ) ) 1 + δ 0 4 + 2 ω p ( 4 R ) d x 1 1 + δ 0 4 C R n + C R n B 2 R ( y ) F ( x , D u ) 1 + δ 0 4 + 2 ω p ( 4 R ) d x 1 1 + δ 0 4 .

Combining (4.15), (4.16), and (4.17), using Proposition 3.8, we obtain

(4.18) R ( u , B R ( y ) ) ( u , B R ( y ) ) C ω p ( 2 R ) R n + R n B R ( y ) F ( x , D u ) 1 + δ 0 4 + 2 ω p ( 4 R ) d x 1 1 + δ 0 4 C ω p ( 2 R ) R n + R n B 2 R ( y ) F ( x , D u ) d x 1 + δ 0 4 + 2 ω p ( 4 R ) 1 + δ 0 4 C ω p ( 2 R ) R n + R n 1 + δ 0 4 ω p ( 4 R ) B 2 R ( y ) F ( x , D u ) d x 1 + δ 0 4 + 2 ω p ( 4 R ) 1 + δ 0 4 C ω p ( 2 R ) R n + B 2 R ( y ) F ( x , D u ) d x .

Let us point out that we use the boundedness of r ω p ( r ) that can be deduced from Assumption (1.5). The constant C on the last line depends also on K F ( x , D u ) d x , which can be regarded as a given constant since u locally minimizes F ( x , D u ) d x .

Next, let us estimate the second part of (4.8), that is, ( v , B R ( y ) ) R ( v , B R ( y ) ) . As we observed in (4.16), for some ε ( 0 , 1 ) we have u W 1 , p 2 ( 2 R ) ( 1 + ε ) ( B R ( y ) ) . So, by virtue of Proposition 3.10, v is also in the class W 1 , p 2 ( 2 R ) ( 1 + ε ) ( B R ( y ) ) and satisfies (3.28) with δ = ε for some ε ( 0 , ε ) . For the sake of simplicity, in the following we rewrite this quantity ε as ε . Mentioning the above remark, we can proceed as the previous calculation and obtain the estimates given from (4.16) and (4.17) by replacing u by v . Thus, we can estimate ( v , B R ( y ) ) R ( v , B R ( y ) ) as follows:

(4.19) ( v , B R ( y ) ) R ( v , B R ( y ) ) C ω p ( 2 R ) R n + R n B R ( y ) F ( x , D v ) 1 + δ 0 4 + 2 ω p ( 4 R ) d x 1 1 + δ 0 4 C ω p ( 2 R ) R n + R n B R ( y ) F ( x , D u ) 1 + δ 0 4 + 2 ω p ( 4 R ) d x 1 1 + δ 0 4 C ω p ( 2 R ) R n + R n B 2 R ( y ) F ( x , D u ) d x 1 + δ 0 4 + 2 ω p ( 4 R ) 1 + δ 0 4 C ω p ( 2 R ) R n + R n 1 + δ 0 4 ω p ( 4 R ) B 2 R ( y ) F ( x , D u ) d x 1 + δ 0 4 + 2 ω p ( 4 R ) 1 + δ 0 4 C ω p ( 2 R ) R n + B 2 R ( y ) F ( x , D u ) d x .

We point out that in the second inequality, we use (3.28).

Now, combining (4.8), (4.18), and (4.19), we can estimate I of (4.7) by the left-hand side of (4.19) (or equivalently (4.18)). On the other hand, as mentioned after (4.7), I I in (4.7) can be estimated by (4.6). Thus, we can see that the following estimate holds, for ρ ( 0 , R ) ,

B ρ ( y ) ( 1 + F ( x , D u ) ) d x B ρ ( y ) ( 1 + F R ( x , D u ) ) d x C ρ R n γ + ω p ( 2 R ) B 2 R ( y ) ( 1 + F ( x , D u ) ) d x + C ω p ( 2 R ) R n .

Since the above estimate holds for ρ [ R , 2 R ) with suitably changed constants, replacing 2 R by R and changing constants, we obtain

B ρ ( y ) ( 1 + F ( x , D u ) ) d x C ρ R n γ + ω p ( R ) B R ( y ) ( 1 + F ( x , D u ) ) d x + C ω p ( R ) R n .

Now, using Lemma 3.1, for any λ ( γ , n ) , we obtain the following decay estimate:

(4.20) B ρ ( y ) ( 1 + F ( x , D u ) ) d x C ρ R n λ B R ( y ) ( 1 + F ( x , D u ) ) d x + C ρ n λ .

Here, since we can choose γ ( 0 , n ) arbitrarily, the above estimate holds for any λ ( 0 , n ) . Thus, for p 0 = inf Ω p ( x ) , we have the following Morrey-type estimate, for every λ ( 0 , n ) ,

B r ( y ) D u p 0 d x C r n λ .

For any α ( 0 , 1 ) , choosing λ = p 0 p 0 α , from the above inequality we conclude that u C loc 0 , α ( Ω ) .

Part 2. Now, we are going to show the Hölder continuity of the gradient D u . From here on, let us assume that p ( ) and a ( ) are Hölder continuous. Particularly, we assume that, for some constants σ ( 0 , 1 ) and L p > 0 , the modulus of continuity of p ( ) , that is, ω p ( ) satisfies ω p ( t ) L p t σ for any t [ 0 , ) . Let us keep in mind our choice of K , R 1 , x 0 , y , and R that is in the beginning part of the proof.

For s ( 0 , R 2 ) we consider a frozen functional s which is defined by (4.1) and (4.2) replacing R with s and taking p 2 = p 2 ( y , s ) . Let v be a minimizer for s with a boundary condition v = u on B s . Then, using the estimate given by Baroni-Colombo-MIngione in [7, p.28] with Ω = B s ( y ) and Ω = B r for some r ( 0 , s ) , we have that, there exist constants ν ( 0 , 1 ) and C > 0 depending only on n , p 2 ( y , s ) , sup a ˜ and R s such that

(4.21) B ρ ( y ) D v ( D v ) ρ p 2 ( y , 2 s ) d x c ρ ν B r ( y ) ( 1 + F s ( x , D v ) ) d x .

On the other hand, by virtue of the minimality of v , using Proposition 3.8 and (4.20) (with ρ = r ), for any λ ( 0 , n ) , we have

(4.22) B r ( y ) F s ( x , D v ) d x B r ( y ) F s ( x , D u ) d x B r ( y ) ( 1 + F ( x , D u ) ) 1 + δ 0 d x C B 2 r ( y ) ( 1 + F ( x , D u ) ) d x 1 + δ 0 r R λ B R ( y ) ( 1 + F ( x , D u ) ) d x + r λ 1 + δ 0 C ( data , R , ( u , K ) ) r λ ( 1 + δ 0 ) .

From (4.21) and (4.22), mentioning that 0 < ρ < r < 1 and choosing λ ( 0 , n ) so that λ ( 1 + δ 0 ) = ν 2 , we obtain

B ρ ( y ) D v ( D v ) ρ p 2 ( y , 2 s ) d x C ρ n + ν r 1 λ ( 1 + δ 0 ) C ρ n + ν 2 .

In what follows, we abbreviate p 2 ( y , 2 s ) p 2 . For t > 0 let us put

f p 2 ( t ) t p 2 , f log ( t ) t p 2 log ( e + t ) , V p 2 ( ξ ) = f p 2 ( ξ ) ξ 1 2 ξ , V log ( ξ ) = f log ( ξ ) ξ 1 2 ξ .

Then for the above quantities, (4.3) and (4.4) are valid by replacing f R by f p 2 or by f log . Also, we mention that

f s ( t ) = f p 2 ( t ) + ( a ¯ ( x ) ) p 2 f log ( t ) .

For p 2 2 , since f p 2 t = p 2 ( p 2 1 ) t p 2 2 and ( a ¯ ( x ) ) p 2 f log ( t ) 0 , we have

ξ η p 2 C ξ η 2 f p 2 ( ξ + η ) ξ η 2 f s ( ξ + η ) .

So, we have that

B s D u D v p 2 d x C B s D u D v 2 f s ( D u + D v ) d x .

The right-hand side of the above inequality coincides to I of (4.7), and, therefore, as mentioned after (4.19), it can be estimated as

(4.23) B s D u D v p 2 d x C ω p ( 2 s ) s n + B 2 s ( y ) F ( x , D u ) d x .

For 2 > p 2 > 1 , from (4.4) we have that

ξ η 2 C V p 2 ( ξ ) V p 2 ( η ) 2 ( f p 2 ( ξ + η ) ) 1 C V p 2 ( ξ ) V p 2 ( η ) 2 ( ξ + η ) 2 p 2 ,

and, therefore, we gain

ξ η p 2 C V p 2 ( ξ ) V p 2 ( η ) p 2 ( ξ + η ) p 2 ( 2 p 2 ) 2 . .

Using the above inequality, Hölder’s inequality, (4.4), and the minimality of v , we obtain

B s D u D v p 2 d x C B s V p 2 ( D u ) V p 2 ( D v ) p 2 ( D u + D V ) p 2 ( 2 p 2 ) 2 d x C B s V p 2 ( D u ) V p 2 ( D v ) 2 d x p 2 2 B s ( D u + D v ) p 2 d x ( 2 p 2 ) 2 C B s ( D u + D v ) p 2 2 D u D v 2 d x p 2 2 B s F s ( x , D u ) d x + B s F s ( x , D v ) d x ( 2 p 2 ) 2 C B s D u D v 2 f p 2 ( D u + D v ) d x p 2 2 B s F s ( x , D u ) d x ( 2 p 2 ) 2 C B s D u D v 2 f 0 ( D u + D v ) d x p 2 2 B s F s ( x , D u ) d x ( 2 p 2 ) 2 C ( A ) p 2 2 ( B ) ( 2 p 2 ) 2 ,

recalling that f p 2 ( t ) f s ( x , t ) .

As in the previous case, ( A ) coincides with I of (4.7). So, ( A ) can be estimated by the right-hand side of (4.23).

We would like to estimate ( B ) by the integral of F ( x , D u ) (not F 0 ( x , D u ) ). Let δ 0 be a positive constant chosen as in Proposition 3.8 and choose R > 0 sufficiently small so that ω p ( 4 R ) < δ 0 . Then, mentioning that 1 log ( e + D u ) 1 + D u 2 + D u p ( x ) and using (3.17), we have

( B ) = B s F s ( x , D u ) d x = B s ( D u p 2 + ( a ¯ D u ) p 2 log ( e + D u ) ) d x C B s ( [ 1 + D u p ( x ) ( 1 + ω p ( 4 s ) ) ] + [ 1 + ( a ¯ D u ) p ( x ) ( 1 + ω p ( 4 s ) ) ] ( log ( e + D u ) ) 1 + ω p ( 4 s ) ) d x C B s ( 1 + ( F ( x , D u ) ) 1 + ω p ( 4 s ) ) d x C s n + C R ω p ( 4 s ) n B 2 s F ( x , D u ) d x 1 + ω p ( 4 s ) . C s n + C s ω p ( 4 s ) n B 2 s F ( x , D u ) d x C s n + C B 2 s ( y ) F ( x , D u ) d x ,

where we apply the boundedness of s ω p ( 4 s ) , and recalling that the second constant of the last line depends, also, on ( u ; K ) . Thus, mentioning that R < 1 , we obtain

(4.24) B s D u D v p 2 d x C ω p ( 2 s ) R n + B 2 s R ( y ) F ( x , D u ) d x p 2 2 s n + s δ 0 n B 2 s F ( x , D u ) d x ( 2 p 2 ) 2 C ω p ( 2 s ) p 2 2 s n ( 1 + ε ) + s δ 0 n B 2 s F ( x , D u ) d x .

In addition, taking s > 0 sufficiently small, we can assume that ω p ( 2 s ) < 1 , and, therefore, the right-hand side of (4.23) can be dominated by the last line of the above estimate. So, we see that (4.24) holds for any p 2 > 1 . Thus, we obtain, for any p 2 > 1 , that

(4.25) B s D u D v p 2 d x C s p 2 2 σ + n + s p 2 2 σ B 2 s F ( x , D u ) d x .

Replacing, in (4.20), ρ and R by 2 s and some fixed R > 2 s with and B R ( y ) K , we have

B 2 s F ( x , D u ) d x C s n λ .

So, from (4.25) and the estimates we obtain

(4.26) B s D u D v p 2 d x C s p 2 2 σ + n + C s p 2 2 σ + n λ .

Bearing in mind that we can choose λ ( 0 , n ) arbitrarily and that we can take ν of (4.21) sufficiently small such that σ > 2 ν , we can select ν and λ such that

(4.27) n λ + 1 2 σ > n + ν 2 .

Now, using (4.21) and (4.26), we obtain that

B ρ D u ( D u ) ρ p 2 d x C B ρ D u ( D v ) ρ p 2 d x C B ρ D v ( D v ) ρ p 2 d x + C B s D u D v p 2 d x C ρ n + ν + C s n λ + 1 2 σ ,

for any ρ < R 2 < R 0 8 . For k > 1 let us set ρ = R k 2 ( R = ( 2 ρ ) 1 k ) , then, from the above estimate, we obtain

B ρ D u ( D u ) ρ p 2 d x C ρ n + ν 2 + C ( 2 ρ ) 2 n 2 λ + σ 2 k .

Fixing

k = 2 n 2 λ + σ 2 n + ν

(the first inequality of (4.27) guarantees that the above choice of k satisfies k > 1 ), we obtain

B ρ D u ( D u ) ρ p 2 d x C ρ n + ν 2 .

By Hölder’s inequality, from the above estimate, we obtain

B ρ ( y ) D u ( D u ) ρ p 0 C ρ p 0 ν 2 p 2 C ρ p 0 ν 2 p 3 .

Now, by Campanato’s theorem, we conclude that D u is Hölder continuous.□

Acknowledgment

The authors are deeply grateful to Giuseppe Mingione for getting them to be interested in the problem treated in this article. They also thank the anonymous reviewers for their careful reading and useful comments.

  1. Funding information: Atsushi Tachikawa is supported by Japan Society for the Promotion of Science KAKENHI Grant Number 20K03707. Maria Alessandra Ragusa is a member of INdAM (Istituto Nazionale di Alta Matematica “Francesco Severi”) Research group GNAMPA (Gruppo Nazionale per l’Analisi Matematica, la Probabilit‘a e le loro Applicazioni).

  2. Author contributions: Maria Alessandra Ragusa: Writing, Editing and Reviewing, Atsushi Tachikawa: Writing, Editing and Reviewing.

  3. Conflict of interest: Maria Alessandra Ragusa is a member of the Editorial Board of the journal, but it does not affect the peer-review process and the final decision. The second author declares non conflict of interest.

References

[1] E. Acerbi and G. Mingione, Regularity results for a class of functionals with non-standard growth, Arch. Ration. Mech. Anal. 156 (2001), no. 2, 121–140. Search in Google Scholar

[2] E. Acerbi and G. Mingione, Regularity results for a class of quasiconvex functionals with nonstandard growth, Ann. Scuola Norm. Sup. Pisa Cl. Sci. (4) 30 (2001), no. 2, 311–339. Search in Google Scholar

[3] E. Acerbi and G. Mingione, Regularity results for electrorheological fluids: the stationary case, C. R. Math. Acad. Sci. Paris 334 (2002), no. 9, 817–822. Search in Google Scholar

[4] E. Acerbi and G. Mingionem, Regularity results for stationary electro-rheological fluids, Arch. Ration. Mech. Anal. 164 (2002), no. 3, 213–259. Search in Google Scholar

[5] P. Baroni, Gradient continuity for p(x)-Laplacian systems under minimal conditions on the exponent, J. Differential Equations 367 (2023), 415–450. Search in Google Scholar

[6] P. Baroni, M. Colombo, and G. Mingione, Harnack inequalities for double phase functionals, Nonlinear Anal. 121 (2015), 206–222. Search in Google Scholar

[7] P. Baroni, M. Colombo, and G. Mingione, Non-autonomous functionals, borderline cases and related function classes, St. Petersburg Math. J. 27 (2016), no. 3, 47–379. Search in Google Scholar

[8] P. Baroni, M. Colombo, and G. Mingione, Regularity for general functionals with double phase, Calc. Var. Partial Differential Equations 57 (2018), no. 2, Art. 62, 48. Search in Google Scholar

[9] P. Baroni and A. Coscia, Gradient regularity for non-autonomous functionals with Dini or non-Dini continuous coefficients, Electron. J. Differential Equations 80 (2022), 30. Search in Google Scholar

[10] A. Benyaiche, P. Harjulehto, P. Hästö, and A. Karppinen, The weak Harnack inequality for unbounded supersolutions of equations with generalized Orlicz growth, J. Differential Equations 275 (2021), 790–814. Search in Google Scholar

[11] I. Chlebicka, C. De Filippis, and L. Koch, Boundary regularity for manifold constrained p(x)-harmonic maps, J. Lond. Math. Soc. (2) 104 (2021), no. 5, 2335–2375. Search in Google Scholar

[12] M. Colombo and G. Mingione, Regularity for double phase variational problems, Arch. Ration. Mech. Anal. 215 (2015), no. 2, 443–496. Search in Google Scholar

[13] M. Colombo and G. Mingione, Bounded minimisers of double phase variational integrals, Arch. Ration. Mech. Anal. 218 (2015), no. 1, 219–273. Search in Google Scholar

[14] M. Colombo and G. Mingione, Calderón-Zygmund estimates and non-uniformly elliptic operators, J. Funct. Anal. 270 (2016), no. 4, 1416–1478. Search in Google Scholar

[15] A. Coscia and G. Mingione, Hölder continuity of the gradient of p(x)-harmonic mappings, C. R. Acad. Sci. Paris Sér. I Math. 328 (1999), no. 4, 363–368. Search in Google Scholar

[16] A. Crespo-Blanco, L. Gasiński, P. Harjulehto, and P. Winkert, A new class of double phase variable exponent problems: existence and uniqueness, J. Differential Equations 323 (2022), 182–228. Search in Google Scholar

[17] C. De Filippis, Higher integrability for constrained minimizers of integral functionals with (p,q)-growth in low dimension, Nonlinear Anal. 170 (2018), 1–20. Search in Google Scholar

[18] C. De Filippis, Partial regularity for manifold constrained p(x)-harmonic maps, Calc. Var. Partial Differential Equations 58 (2019), no. 2, Art. 47, 38. Search in Google Scholar

[19] C. De Filippis, Gradient bounds for solutions to irregular parabolic equations with (p,q)-growth, Calc. Var. Partial Differential Equations 59 (2020), no. 5, Paper No. 171, 32. Search in Google Scholar

[20] C. De Filippis, Optimal gradient estimates for multi-phase integrals, Math. Eng. 4 (2022), no. 5, Paper No. 043, 36. Search in Google Scholar

[21] C. De Filippis and F. Leonetti, Uniform ellipticity and (p,q) growth, J. Math. Anal. Appl. 501 (2021), no. 1, Paper No. 124451, 11. Search in Google Scholar

[22] C. De Filippis and G. Mingione, Manifold constrained non-uniformly elliptic problems, J. Geom. Anal. 30 (2020), no. 2, 1661–1723. Search in Google Scholar

[23] C. De Filippis and G. Mingione, On the regularity of minima of non-autonomous functionals, J. Geom. Anal. 30 (2020), no. 2, 1584–1626. Search in Google Scholar

[24] C. De Filippis and G. Mingione, Interpolative gap bounds for nonautonomous integrals, Anal. Math. Phys. 11 (2021), no. 3, Paper No. 117, 39. Search in Google Scholar

[25] C. De Filippis and G. Mingione, Lipschitz bounds and nonautonomous integrals, Arch. Ration. Mech. Anal. 242 (2021), no. 2, 973–1057. Search in Google Scholar

[26] C. De Filippis and G. Palatucci, Hölder regularity for nonlocal double phase equations, J. Differential Equations 267 (2019), no. 1, 547–586. Search in Google Scholar

[27] L. Diening and F. Ettwein, Fractional estimates for non-differentiable elliptic systems with general growth, Forum Math. 20 (2008), no. 3, 523–556. Search in Google Scholar

[28] M. Eleuteri, Hölder continuity results for a class of functionals with non-standard growth, Boll. Unione Mat. Ital. Sez. B Artic. Ric. Mat. eight 7 (2004), no. 1, 129–157. Search in Google Scholar

[29] F. Giannetti, A. P. di Napoli, and A. Tachikawa, Partial and full boundary regularity for non-autonomous functionals with Φ-growth conditions, Forum Math. 31 (2019), no. 4, 1027–1050. Search in Google Scholar

[30] F. Giannetti and A. Passarelli di Napoli, Regularity results for a new class of functionals with non-standard growth conditions, J. Differential Equations 254 (2013), no. 3, 1280–1305. Search in Google Scholar

[31] F. Giannetti, A. Passarelli di Napoli, and A. Tachikawa, Partial regularity results for non-autonomous functionals with Φ-growth conditions, Ann. Mat. Pura Appl. (4) 196 (2017), no. 6, 2147–2165. Search in Google Scholar

[32] M. Giaquinta and L. Martinazzi, An introduction to the regularity theory for elliptic systems, harmonic maps and minimal graphs, volume 11 of Appunti. Scuola Normale Superiore di Pisa (Nuova Serie) [Lecture Notes. Scuola Normale Superiore di Pisa (New Series)]. Edizioni della Normale, Pisa, second edition, 2012. Search in Google Scholar

[33] M. Giaquinta and G. Modica, Regularity results for some classes of higher order nonlinear elliptic systems, J. Reine Angew. Math. 311/312 (1979), 145–169. Search in Google Scholar

[34] M. Giaquinta, G. Modica, and J. Souček, Cartesian currents in the calculus of variations. II, volume 38 of Ergebnisse der Mathematik und ihrer Grenzgebiete. 3. Folge. A Series of Modern Surveys in Mathematics [Results in Mathematics and Related Areas. 3rd Series. A Series of Modern Surveys in Mathematics]. Springer-Verlag, Berlin, 1998. Variational integrals. Search in Google Scholar

[35] E. Giusti, Direct Methods in the Calculus of Variations, World Scientific Publishing Co. Inc., River Edge, NJ, 2003. Search in Google Scholar

[36] P. Harjulehto and P. Hästö, Double phase image restoration, J. Math. Anal. Appl. 501 (2021), no. 1, Paper No. 123832, 12. Search in Google Scholar

[37] T. Iwaniec and G. Martin, Geometric function theory and non-linear analysis, Oxford Mathematical Monographs, The Clarendon Press, Oxford University Press, New York, 2001. Search in Google Scholar

[38] T. Iwaniec and A. Verde, On the operator L(f)=flog∣f∣, J. Funct. Anal. 169 (1999), no. 2, 391–420. Search in Google Scholar

[39] J. Mal&#1acute; and W. P. Ziemer, Fine regularity of solutions of elliptic partial differential equations, volume 51 of Mathematical Surveys and Monographs. American Mathematical Society, Providence, RI, 1997. Search in Google Scholar

[40] P. Marcellini, Regularity of minimizers of integrals of the calculus of variations with nonstandard growth conditions. Arch. Rational Mech. Anal. 105 (1989), no. 3, 267–284. Search in Google Scholar

[41] P. Marcellini, Regularity and existence of solutions of elliptic equations with p,q-growth conditions, J. Differential Equations 90 (1991), no. 1, 1–30. Search in Google Scholar

[42] P. Marcellini, Everywhere regularity for a class of elliptic systems without growth conditions, Ann. Scuola Norm. Sup. Pisa Cl. Sci. (4) 23 (1996), no. 1, 1–25. Search in Google Scholar

[43] G. Mingione and V. Rădulescu, Recent developments in problems with nonstandard growth and nonuniform ellipticity, J. Math. Anal. Appl. 501 (2021), no. 1, Paper No. 125197, 41. Search in Google Scholar

[44] M. A. Ragusa and A. Tachikawa, Boundary regularity of minimizers of p(x)-energy functionals, Ann. Inst. H Poincaré Anal. Non Linéaire 33 (2016), no. 2, 451–476. Search in Google Scholar

[45] M. A. Ragusa and A. Tachikawa, Regularity for minimizers for functionals of double phase with variable exponents, Adv. Nonlinear Anal. 9 (2020), 710–728. Search in Google Scholar

[46] M. A. Ragusa, A. Tachikawa, and H. Takabayashi, Partial regularity of p(x)-harmonic maps, Trans. Amer. Math. Soc. 365 (2013), no. 6, 3329–3353. Search in Google Scholar

[47] M. Růžička, Electrorheological fluids: modeling and mathematical theory, volume 1748 of Lecture Notes in Mathematics, Springer-Verlag, Berlin, 2000. Search in Google Scholar

[48] X. Shi, V. D. Rădulescu, D. D. Repovš, and Q. Zhang, Multiple solutions of double phase variational problems with variable exponent, Adv. Calc. Var. 13 (2020), no. 4, 385–401. Search in Google Scholar

[49] A. Tachikawa, On the singular set of minimizers of p(x)-energies, Calc. Var. Partial Differential Equations 50 (2014), no. 1–2, 145–169. Search in Google Scholar

[50] A. Tachikawa, Boundary regularity of minimizers of double phase functionals, J. Math. Anal. Appl. 501 (2021), no. 1, 123946. Search in Google Scholar

[51] A. Tachikawa and K. Usuba, Regularity results up to the boundary for minimizers of p(x)-energy with p(x)>1, Manuscripta Math. 152 (2017), no. 1–2, 127–151. Search in Google Scholar

[52] J. Zhang, W. Zhang, and V. D. Rădulescu, Double phase problems with competing potentials: concentration and multiplication of ground states, Math. Z. 301 (2022), no. 4, 4037–4078. Search in Google Scholar

[53] V. V. Zhikov, On Lavrentievas phenomenon, Russian J. Math. Phys. 3 (1995), no. 2, 249–269. Search in Google Scholar

[54] V. V. Zhikov, On the averaging of nonlinear variational problems in punctured domains, Dokl. Akad. Nauk 345 (1995), no. 2, 156–160. Search in Google Scholar

[55] V. V. Zhikov, On the Lavrentiev effect, Dokl. Akad. Nauk 345 (1995), no. 1, 10–14. Search in Google Scholar

[56] V. V. Zhikov, On some variational problems, Russian J. Math. Phys. 5 (1997), 105–116. Search in Google Scholar

Received: 2023-07-13
Revised: 2023-10-11
Accepted: 2024-05-06
Published Online: 2024-06-13

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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